Cooling rate effects on the magnetization of volcanic rocks: Some implications for paleointensity determination

Effects of variation of cooling rate in the acquisition of thermoremanent magnetization (TRM) are analyzed on a suite ofvolcanic rocks. We use a three-step cooling rate experimental procedure applied at three distinct temperatures of TRM acquisition.Sixteen selected, thermally stable samples from La...

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Detalles Bibliográficos
Autores: Juan Morales, Avto Goguitchaichvili, Jaime Urrutia-Fucugauchi
Tipo de recurso: artículo
Estado:Versión publicada
Fecha de publicación:2006
País:México
Institución:Universidad Nacional Autónoma de México
Repositorio:Redalyc-UNAM
OAI Identifier:oai:redalyc.org:56845205
Acceso en línea:https://www.redalyc.org/articulo.oa?id=56845205
Access Level:acceso abierto
Palabra clave:Ciencias de la Tierra
Cooling rate
paleointensity
volcanic rocks
rock magnetism
Descripción
Sumario:Effects of variation of cooling rate in the acquisition of thermoremanent magnetization (TRM) are analyzed on a suite ofvolcanic rocks. We use a three-step cooling rate experimental procedure applied at three distinct temperatures of TRM acquisition.Sixteen selected, thermally stable samples from Late Quaternary lava flows were given a pTRM (300°C) at a slow cooling rate.The acquired intensities were measured at room temperature. A second pTRM was applied to the same specimens using a fastcooling rate, and the acquired intensities were measured at room temperature. Finally a third pTRM was induced as in the firststep, using a slow cooling rate. The procedure was repeated to create pTRM’s at higher temperatures of 450° and 550°C.Corresponding percent variations between magnetization intensities acquired at slow-fast and at slow-slow cooling rates werecalculated to investigate the influence of cooling rate on TRM intensity acquisition, and on TRM acquisition capacity. Weobserve values as high as 300 % in the former case (300 °C). Intensity of the ancient geomagnetic field obtained from volcanicrocks could be overestimated by at least 15% due to a variation in cooling rate normally employed in the laboratory, as comparedto slower rates found in nature.